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John E. Kosin
RMI Company - U.S.A.
TREND IN PROCESSING, FABRICATION AND APPLICATION OF TITANIUM
1 - INTRODUCTION
Prior to discussion of the text of my presentation this
morning, I would like to review the availability and properties
of titanium (Fig. 1).
Titanium is not a rare element. In fact, you can see (Fig. 2)
that titanium is the fourth most abundant metal in the earth's
crust, following after aluminium, iron and magnesium.
Titanium is well dispersed throughout the earth and, as you can
see in Fig. 3, there are workable deposits of titanium ore
throughout the globe. Thus, it is not sensitive to geographical
or political problems that may exist in the world.
Fig. 4 shows the growth of the titanium industry by markets in
the United States from 1966 through 1985.
The free world consumption of titanium would be about twice the
numbers you see here. As you see, the defence usage has been
fairly constant over the period. Significant growth has
occurred in the commercial aerospace and industrial markets
since about 1976.
From Fig. 5 you can also see that the projected free world
capacity exceeds the demand. This is further illustrated
(Fig. 6) when one considers that only 5% of the TiO2
consumption goes into metal production.
8
So we might ask, if titanium is so abundant, if it is so well
dispersed, why is it not used more?
The growth of titanium has been restricted to a certain extent
by the cost of the metal, cost of winning it from the ore. It
is fairly expensive in terms of energy. However, there has been
a gradual decrease in the amount of energy.
There has also been a rather large increase in the usage of
titanium.
So it seem reasonable to expect that the driving force for
changing trends in material use is to design around the key
properties of titanium, improve the performance and operating
costs, while at the same time, reducing the manufacturing
costs.
The key properties (Fig. 7) of titanium are fairly well known.
To review, they centre around two characteristics. First of
all, corrosion resistance. Titanium has excellent corrosion
resistance in all natural media, including chlorides and
organics, very resistant to salt water and chloride solutions.
The second main characteristic is that it has a low density,
about one-half that of iron and slightly higher than aluminium.
However the metal, as you can see, has high strength
capabilities. So, when you combine the low density with high
strength, you have a very efficient engineering material.
Another favourable characteristic of titanium includes its high
temperature strength.
Other interesting properties that, on occasion, are very useful
in design applications include:
9
- it has very good ballistic resistance;
- it has low thermal expansion, which is very similar to
that of glass and composites, so it is very compatible
with those materials;
- it has a low elastic modulus, which makes it a unique
spring material, a very efficient spring material;
- it has, on the corrosion side, good heat transfer;
- it is very effective in heat exchangers.
Titanium also has some very unique electrochemical
characteristics, and it also has a very short radioactive
half-life, which can be useful in processing uranium and spent
uranium. I will expand on some examples of these properties
later in my presentation.
With this in mind, I would like to review the trends in
processing, fabrication and applications. Since time does not
permit me to cover all aspects, I will elaborate only on those
areas of major activity in the USA during the past three years.
2 - PROCESSING TRENDS
Responding to the aerospace, chemical process and electronic
industries needs for high-cleanliness, high purity titanium,
nonconsumable, cold-hearth melting is receiving a lot of
attention. The key is cold-hearth as opposed to drip-melting
directly into a cold-wall mold.
Production of these high performance engineering materials
requires highly controlled processing conditions. Both demands of
high purity processing environment and high performance
heating source can be met using:
- Electron Beam
- Plasma
10
melting conditions. These technologies are similar with regard
to hearth melting.
Electron-beam melting (Fig. 8) is a vacuum process which
utilizes the thermal energy of the electron beam for melting
and refining operations. The heat in the prevailing vacuum
environment permits distillation of volatile elements including
vaporization of suboxides, evolution and removal of gases, and
vaporization of metal impurities with vapour pressures above
that of the titanium. Most notable in titanium is aluminium,
since it is common to most alloy systems.
Alec Mitchell of the University of British Columbia is working
on inline compositional analyses aimed at making compositional
adjustments during the melting process. Using the principles of
energy dispersion analysis (EDS), Mitchell has done pioneering
work in this area. The x-rays that generate the information are
excited by the very energetic beam which is used to heat the
surface of the liquid metal. Fig. 9 is an installation and
Fig. 10 is the molten pool and metal cascading over the hearth
into the mold.
Plasma-melting can be performed with a cold-hearth as well, but
in an inert gas atmosphere in the pressure range of 150 mbar
and 2 bar. Hence, one does not get the ultimate refinement as
with a vacuum system.
Electron-beam melting is the only process which simultaneously
can take advantage of the cold-hearth effect and the refining
effect of high and ultra-high vacuum.
Almost since its commercial inception, prompted by the
development of the gas turbine in the mid-forties, titanium has
been plagued by a defect (Fig. 11) known as:
11
Type 1
LDI - low density inclusion
Hard Alpha
IRI - Interstitially Rich Inclusion
This defect is characterized by high hardness and higher
melting point, its composition is higher in nitrogen, may also
be higher in oxygen, and is usually depleted in major alloying
elements. Although it is denser (approximately 15%) than molten
titanium, it derives its low density connotation from the fact
that it is usually associated with a void. It acts as a crack
initiator and results in a premature fatigue failure.
Although an additional CEVAM has greatly reduced the incidence,
inspection techniques, namely ultrasonic, which has also
improved in the level of detection over the period, still
remains as the last chance of preventing a defect from getting
into the field.
Hence, the interest in hearth-melting, since defects that are
denser than the molten metal will sink to the bottom and become
entrapped in the skull which lines the hearth.
The procedure for removal of these denser materials has been coined
Defect-Free Titanium (DFT).
Commercially, hearth-melting is very attractive for
consolidation of scrap that otherwise would not be suitable by
CEVAM. In particular, small pieces and machining chips that are
generated with carbide tooling.
CEVAM (Fig. 12 and Fig. 13) begins with the fabrication of
electrodes (Fig. 14) made up of compressed sponge compacts
containing the alloy additions. Chemically compatible scrap can
become part of the electrode makeup, but they are rather large
12
in size because they must be individually affixed to the
electrode. Smaller pieces can be included in the compact, but
such additions are limited by the compact strength. One can
also add limited quantities during the melting process by means
of a side-feeder.
With this type of scrap processed through a cold-hearth, any
segment of the electrode cross-section can be cast as dictated
by the mold-configuration. Hence, the attractiveness of a
combined nonconsumable hearth and CEVAM ingot.
This is reflected in the increased titanium scrap consumption
in ingot (Fig. 15) for the period 82-86.
Thus, one can take advantage of the refinement afforded through
cold-hearth melting and satisfy most industry specifications
with subsequent CEVAM melts since alloys shall be multiple
melted under vacuum or inert gas with the last melting cycle
under vacuum.
3 - FABRICATION TRENDS
In fabrication, I would like to discuss two areas, namely:
- Forging;
- Superplastic Forming and/or Diffusion Bonding.
Forging
I will discuss forging from two perspectives: 1) from what is
happening in the USA; 2) this combined with forging of
titanium.
13
Thus, all my remarks relate to trends in the USA forging
industry as related to only titanium forgings. First I will
discuss the most popular titanium alloys used by the U.S.
forging industry; this will be followed by a brief description
of several developmental alloys. Second, I will discuss
developmental forging techniques related to attaining net shape
and improved properties. Illustrations n. 16 and 17 contain
information of general interest to forgers on current popular
titanium alloys. Included is the transformation temperature,
the forging range, the pressures required and the general
cracking resistance.
The alloys are classified in three primary groups: the alpha,
the alpha-beta and the new beta. As the beta increases the
cracking resistance improves, the transformation temperature
decreases, the forging temperature decreases, and the pressure
required decreases. As a result I suppose it is not surprising
that several near beta alloys have been used or considered for
forging applications. These include: 10V 2Fe 3Al (10-2-3)
transage alloys and the 38-6-44 or BetaC alloy. The importance
of this newer materials will be evident shortly when we discuss
the advances in the forging techniques (Fig. 18). Most of the
conventional forging methods can be applied to titanium and the
titanium alloys: forging, hammer forging, ring rolling,
mechanical or screw press forging. Because of the influence of
the die chilling on the deformation characteristics,
properties, structure and surface cracking, the conventional
forging process does have significant liabilities. This has
led to appreciable interest in technologies utilizing hot dies
which have an added benefit of achieving near or net shapes.
Let us now review two key differences in conventional, on the
left, versus net shape forging, on the right. These are:
- Structure/Property
- Product Yield/Cost
14
Fig. 19 shows studies by Dr. Chen and compares the
macrostructures of Ti-6242Si alloy pancake made by the
different processes. As you can readily see, the macrostructure
becomes increasingly uniform as we progress from conventional
to warm die to isothermal forging.
Most commercial titanium alloys are forged near 1750° F (954°
C). As a result, isothermal forging - meaning die temperatures
near 1750° F (954° C) is extremely difficult since:
- Die materials like IN 100 are unrepairable
- Die heating systems are complicated
- Possibility of oxygen penetration into Ti
Hot die forging is conducted using normal metal temperatures
1750° F (954° C) and die temperature near 1400° F (750° C).
Advantages are:
- wrought alloy dies Astralloy, Waspalloy: lower cost and
weldable
- die heating simpler
- can produce near net and net shape
The impact of this technology is not only in improved structure
control, but in achieving shapes nearer the final
configuration.
Figure 20 illustrates metal utilization for various forging
processes for a typical titanium alloy such as Ti-6Al-4V.
Some examples of near and net shape forgings:
Figure 21: Ti-10-2-3 Near Net Instrument Housing
Figure 22: Ti-6Al-4V Near Net Disc
15
Net shape (Figure 23). In this example, a transage alloy
pressure vessel dome was isothermally forged at 1500° F (800° C).
Top surface with bosses was forged net. Machining was required
only on the top of the bosses to get the desired flatness and
inside the dome which was a simple turning operation.
A cost comparison (Figure 24) of several processes by Kuhlman
of Alcoa shows the advantage of net shape forgings of beta-type
alloys.
This analysis was done on an engine mount and is based upon
production of 100 forgings. In summary, the machined part from
plate is 10% greater than a close-die part. However, the net
10-2-3 is 40% less expensive.
As you can see, new developments are being driven by reduced cost
through net shape forgings or improved performance through
property optimization.
4 - SUPERPLASTIC FORMING/DIFFUSION BONDING
Since superplastic forming and/or diffusion bonding offers
major savings in weight and manufacturing cost, there is
increased interest in the feasibility of applying the
techniques to the manufacture of a range of complex structural
aerospace components.
Diffusion Bonding is sometimes called diffusion welding. It is
a solid state welding process in which the surfaces are placed
in proximity under a moderate pressure at elevated temperature.
Coalescence occurs across the interface. Because diffusion
bonding requires heat, pressure and a vacuum, inert gas or a
reducing atmosphere, equipment is frequently custom built by
the user.
16
Figure 25 is a wing carry through fabricated by diffusion
bonding 533 individual details.
Superplastic forming of titanium plate and sheet was also
developed as a reduced-cost method for processing of material.
From Figure 26, it can be seen that most of the titanium alloys
can be formed superplastically. The M-value or strain rate
sensitivity factor is a measure of superplasticity of the alloy
at a given strain rate. Any value greater than 0.5 is
considered a candidate for superplastic forming. In conjunction
with typical SPF elongation, it can be seen that Ti-6Al-4V is
the most desirable candidate. In Figure 27 one can see the
influence of grain size on flow stress. RMI has a grain size of
5µm. At this grain size, one can see how the flow stress and
M-factor are enhanced for superplastic forming. Figure 28 is
the typical microstructure of RMI sheet. Note that the
microstructures are similar before and after a simulated SPF
cycle.
Figure 29 is an example of the superplastic forming process.
These are examples of free blowing. That is, the final geometry
is not restricted or controlled by dies.
For the sphere, clean and treated sheets are edge-welded to
exclude air, but a pipe is attached for pressurization. After
bringing the unit to temperature, gas pressure, usually argon,
is applied until the desired shape has been achieved.
A combination of superplastic forming and diffusion (SPF/DB) is
being used on titanium to produce complex structures. Figure 30
is an example of the process. The sheets are prepared as with
SPF, except they are treated with stop offs where bonding is
not desired. Initial bonding occurs under pressure at
temperature and then internal pressure, through the pipe,
causes superplastic flow of the outer two sheets to fill the
die and create the configuration shown.
17
Integrally stiffened structures are produced in this manner.
Following are examples (Figures 31, 32 and 33) of some
superplastically formed parts. Note the generally smaller bend
radii, deeper drawability and larger size that can be achieved
as compared to standard hot-formed (Figure 34) parts.
One U.S. aerospace company is superplastically forming a part
that previously consisted of seven individually hot formed
parts that were joined by conventional means, one can really
see the attractiveness of these fabrication methods for
producing hardware.
Spurred by the aerospace industry’s use of titanium discovery
of titanium’s excellent corrosion performance opened up a host
of unique applications for design engineering in the early
1960’s. Titanium corrosion resistance in neutral to oxidizing
environments is mainly due to a surface oxide layer. Engineers
in the chemical process industries, quick to exploit this
characteristic, were the first to apply titanium. At the same
time titanium unique electrochemical characteristics
revolutionized the chloro-alkali industry through the use of
precious metal coated titanium anodes. From these first two
industrial markets, titanium has expanded its non-aerospace
presence into more than 25 distinct market segments.
Figure 35 is the distribution and growth of those markets.
Its weaknesses include poor corrosion resistance to reducing
acids, red fuming, nitric acids and hot organic acids. If we
look at the general properties of titanium there are a few
observations that need to be made (Fig. 36). As one moves
towards the alpha alloys there is improved corrosion to
oxidizing environments at low to moderate strength levels. As
one moves to the beta alloys there is improved corrosion
resistance to reducing environments at higher strength levels.
18
Alloyed versions including small amounts of palladium and
molybdenum increase the titanium resistance to reducing acids.
Additions of aluminum and vanadium increase the strength and
slightly reduce the range in the oxidizing region. But note the
beta alloy, the Beta C (Fig. 37), with the high attainable
strength up to 315° C and the range in both the oxidizing and
reducing sides. In the search for alternate energy sources, it
is not surprising that this alloy is rapidly gaining acceptance
in geothermal and sour gas wells.
5 - GEOTHERMAL
In geothermal, energy is extracted from the earth in the form
of high temperature hypersaline brines. Some of these brines
also contain H2S and CO2 at temperature ranges of 450° - 600° F
(232° - 315° C). These brines impose severe restrictions on
metals with limited corrosion resistance. In addition, high
strength and heat treatability are required due to the large
piping employed. In fact, beta titanium may be the only
economical way to produce energy using geothermal technology.
Figure 38 is an example of geothermal applications.
6 - SOUR GAS
Fossil fuel shortages have forced the oil and gas industries to
produce more corrosive deposits. These deposits typically contain
hydrogen sulphide (hence the term “sour”), pose an exceptional
challenge to the materials engineer.
Figure 39 shows the Beta CTM advantages in the oil field
market. These include high strength, corrosion resistance and
low density, which are all necessary for successful usage. In
addition, the low elastic modulus makes it nearly perfect for
19
Figure 40, one can see the uses of Beta CTM for down-hole
applications.
Figure 41 and 42 are some of the casings and strings being used
in these installations. From their size and quantity, it is
easy to see the tremendous usage potential in these markets.
In summary, titanium usage will continue to grow based upon its
unique combination of properties aided by improved performance
and reduced total cost of the entire system.
20
Fig. 1 - Titanium properties
Fig. 2 - Relative abundance of materials in the heth’s
crust
21
Fig. 3 - Deposits of Titanium ores throughout
the globe
Fig. 4 - Growth of the titanium industry by markets
in the U.S. from 1966 through 1985
22
Fig. 5 - Projected free world capacity and demand
Fig. 6 - Titanium ore consumption
23
Fig. 7 - Titanium key properties
Fig. 8 - Electron beam processes
24
Fig. 9 - Electron beam installation
Fig. 10 - Molten metal flow in the electron beam
cold earth
25
Fig. 11 - Type I defect in titanium
Fig. 12 - Consumable electrode vacuum arc melting
(CEVAM) furnace diagram
26
Fig. 13 - CEVAM furnace at RMI
Fig. 14 - Compressed sponge electrodes
27
Fig. 15 - U.S. scrap consumption trend
Fig. 16 - Forging for titanium alloys
28
Fig. 17 - Forging conditions for titanium alloys
Fig. 18 - Commercial techniques for forging titanium
29
Fig. 19 - Macrostructure comparison in different
Ti-6242Si forgings
Fig. 20 - Metal utilisation for various forging
processes
30
Fig. 21 - 10-2-3 near net shape instrument housing
Fig. 22 - Near net shape disc
31
Fig. 23 - Transage alloy isothermal forging
Fig. 24 - Cost comparison in various fabrication
methods
32
Fig. 25 - Wing carry through structure fabricated by
diffusion bonding
Fig. 26 - SPF characteristics for various Ti alloys
33
Fig. 27 - Influence of grain size on flow stress
Fig. 28 - Typical microstructure of RMI sheet
34
Fig. 29 - Examples of SPF processes
Fig. 30 - A SPF/DB process example
35
Fig. 31 - SPF part
Fig. 32 - SPF part
36
Fig. 33 - SPF part
Fig. 34 - Conventional hot formed parts
37
Fig. 35 - Distribution and growth of titanium
Industrial markets
Fig. 36 - General properties of titanium alloys
38
Fig. 37 - Elevated temperature yield strength vs.
Corrosion resistance for various titanium
Alloys
Fig. 38 - Geothermal applications of titanium alloys
39
Fig. 39 - Beta C advantages in the oil field market
Fig. 40 - Examples of downhole applications for
Beta C alloy
40
Fig. 41 - Beta C downhole piping
Fig. 42 - Beta C downhole piping
41